Low bandgap mid-infrared thermophotovoltaic arrays based on InAs
Introduction
There is continuing interest in thermophotovoltaic (TPV) devices because they can provide an attractive method for the direct conversion of heat into electricity in a wide variety of applications, and in particular for industrial waste heat recovery and silent or remote power generation. The optimum TPV cell bandgap depends on the emitter blackbody temperature, and following the thermodynamic detailed balance model [1], in the ideal case where radiative recombination is dominant, the maximum TPV cell efficiency is ∼35% for source temperatures between 1200 and 2500 K, such that the optimum bandgap falls in the range 0.2–0.5 eV [2]. To date previous work has concentrated on TPV devices matched to high temperature sources using semiconductors with larger bandgaps such as silicon (Eg = 1.1 eV), InGaAs [3] on InP (typically Eg = 0.5–0.73 eV, but which is limited by lattice mismatch to the higher bandgaps), or InGaAsSb on GaSb (constrained to Eg = 0.5 eV by a miscibility gap). There have been some studies of the development and characterisation of InAs based diodes for lower temperature TPV applications, but, these reports concern mainly epitaxial growth and characterisation of individual elements [4], [5]. Meanwhile, although there are currently active investigations into quantum cascade based or multiple-junction TPVs, there are still no TPV arrays capable of electricity generation using thermal source temperatures below 1000 °C [6], [7]. In this work we have developed an approach using InAs with a bandgap of 0.32 eV (300 K) and demonstrate prototype InAs-based TPV arrays. These devices have a lower bandgap than conventional GaSb or InGaAs cells and are well-matched to cooler thermal sources at temperatures ∼500 °C.
Section snippets
Experimental procedures
The TPV cell design implemented here is shown in Fig. 1(a) and comprised a p-type quaternary alloy layer of InAsSbP with bandgap (∼0.5 eV) as a window to allow light into the active region and reduce surface recombination of photo-generated carriers. The InAs undoped active region was ∼6 μm in thickness to provide effective absorption. The epitaxial layers of InAs and quaternary InAsSbP were grown lattice-matched onto a p-type (1 0 0) InAs substrate by conventional liquid phase epitaxy (LPE) using
Results
Fig. 1(b) shows the simulated energy band diagram for the structure at zero bias obtained using SimWindows [10]. The p-InAsSbP window enables long wavelength photons to be absorbed within the undoped InAs active region, but also contributes to the TPV response. As shown in Fig. 1(c) the long wavelength cut-off is determined by the InAs, whereas the InAsSbP effectively extends the short wavelength photoresponse which is limited by the non-radiative recombination of photogenerated carriers at the
Conclusions
We have developed narrow band gap InAs/InAs0.61Sb0.13P0.26 heterojunction photodiode structures for thermophotovoltaic (TPV) electricity generation from (waste) heat sources at temperatures below 1000 °C. For a single element the maximum open circuit voltage (Voc) and short circuit current density (Jsc) were obtained as 0.06 V and 0.89 A cm−2 for a blackbody temperature of 950 °C and an incident power density of 720 mW cm−2. The fill factor obtained was 37% with a corresponding efficiency of 3% with
Conflict of interest
There is no conflict of interest.
Acknowledgements
Financial support for this work was provided by the UK Technology Strategy Board in collaboration with CST Global Ltd., IQE Ltd., Tata Steel and NSG Pilkington Ltd. under Grant Nos: TP11/LCE/6/I/AE096F and TP 14649-88258.
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